EP2202762B1 - Anordnung mit einem supraleitfähigen Kabel - Google Patents

Anordnung mit einem supraleitfähigen Kabel Download PDF

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Publication number
EP2202762B1
EP2202762B1 EP08291180A EP08291180A EP2202762B1 EP 2202762 B1 EP2202762 B1 EP 2202762B1 EP 08291180 A EP08291180 A EP 08291180A EP 08291180 A EP08291180 A EP 08291180A EP 2202762 B1 EP2202762 B1 EP 2202762B1
Authority
EP
European Patent Office
Prior art keywords
conductor
arrangement according
screen
superconducting
cryostat
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Not-in-force
Application number
EP08291180A
Other languages
German (de)
English (en)
French (fr)
Other versions
EP2202762A1 (de
Inventor
Rainer Soika
Mark Stemmle
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nexans SA
Original Assignee
Nexans SA
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority to EP08291180A priority Critical patent/EP2202762B1/de
Application filed by Nexans SA filed Critical Nexans SA
Priority to AT08291180T priority patent/ATE498184T1/de
Priority to DK08291180.1T priority patent/DK2202762T3/da
Priority to DE502008002580T priority patent/DE502008002580D1/de
Priority to US12/623,849 priority patent/US9496072B2/en
Priority to JP2009269977A priority patent/JP5632152B2/ja
Priority to KR1020090124282A priority patent/KR101657600B1/ko
Priority to CN2009102614492A priority patent/CN101752036B/zh
Publication of EP2202762A1 publication Critical patent/EP2202762A1/de
Application granted granted Critical
Publication of EP2202762B1 publication Critical patent/EP2202762B1/de
Not-in-force legal-status Critical Current
Anticipated expiration legal-status Critical

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    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B12/00—Superconductive or hyperconductive conductors, cables, or transmission lines
    • H01B12/02—Superconductive or hyperconductive conductors, cables, or transmission lines characterised by their form
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B12/00—Superconductive or hyperconductive conductors, cables, or transmission lines
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B12/00—Superconductive or hyperconductive conductors, cables, or transmission lines
    • H01B12/16—Superconductive or hyperconductive conductors, cables, or transmission lines characterised by cooling
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B13/00—Apparatus or processes specially adapted for manufacturing conductors or cables
    • H—ELECTRICITY
    • H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02H—EMERGENCY PROTECTIVE CIRCUIT ARRANGEMENTS
    • H02H7/00—Emergency protective circuit arrangements specially adapted for specific types of electric machines or apparatus or for sectionalised protection of cable or line systems, and effecting automatic switching in the event of an undesired change from normal working conditions
    • H02H7/001—Emergency protective circuit arrangements specially adapted for specific types of electric machines or apparatus or for sectionalised protection of cable or line systems, and effecting automatic switching in the event of an undesired change from normal working conditions for superconducting apparatus, e.g. coils, lines, machines
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Definitions

  • the invention relates to an arrangement with a superconducting cable, which consists of a superconductive conductor and a superconductive screen surrounding it concentrically with the interposition of a dielectric and which is surrounded by a free space for passing a coolant from a cryostat, which consists of two concentric with each other arranged metallic tubes between which a vacuum insulation is arranged ( WO 03/052775 A1 ).
  • a superconducting cable in today's technology has electrical conductors of a composite material containing ceramic material which changes to the superconducting state at sufficiently low temperatures.
  • the electrical DC resistance of a correspondingly constructed conductor is zero with sufficient cooling, as long as a certain current is not exceeded.
  • Suitable ceramic materials are, for example, YBCO (yttrium-barium-copper-oxide) or BSCCO (bismuth-strontium-calcium-copper-oxide).
  • Sufficiently low temperatures to bring such a material into the superconductive state are for example between 67 K and 110 K.
  • Suitable coolants are, for example, nitrogen, helium, neon and hydrogen or mixtures of these substances.
  • a superconductive cable with cold dielectric is used. It consists of an inner conductor mounted on a tubular support and a screen arranged concentrically therewith, which are separated from one another by the dielectric (insulation) and kept at a distance.
  • the conductor and the screen are made, for example Tapes of superconductive material, such as YBCO or BSCCO, which are wrapped closely adjacent to each other with a long stroke around a pad.
  • This known superconducting cable is constructed so that the superconducting screen shields the magnetic field of the superconducting conductor to the outside in undisturbed operation.
  • the cable impedance changes only insignificantly. Due to the short-circuit current, a high energy input occurs, both in the conductor and in the shield of the cable, which can lead to the destruction of the cable (burn-out).
  • the invention has for its object to make the initially described arrangement so that the effects of a short circuit can be substantially reduced.
  • the screen consists of a superconducting material whose electrical resistance in the normally conductive state by a factor of at least 50 is higher than the electrical resistance of the material used for the conductor in a normally conductive state.
  • the energy input causes a temperature increase in the cable. Due to this temperature increase and the short-circuit current exceeding the rated current, the superconductive materials of the conductor and the screen transition from their superconducting state to the normally conductive state. Because of its high electrical resistance, the screen will then carry a negligible current so that it loses its shielding effect. As a result, the magnetic field of the conductor can spread out without hindrance. This directly causes a substantial increase in the inductance of the conductor, ie an increase in its electrical impedance. The current flowing through the conductor short-circuit current is characterized noticeably and quickly limited. The occurring in known cables by a high short-circuit current heating is reduced accordingly.
  • the effect of limiting the short-circuit current can be increased by the additional attachment of a layer of ferromagnetic material outside the screen.
  • Ferromagnetic materials which can be used for such a layer are all materials which have a relative permeability ⁇ r greater than 10.
  • the layer of ferromagnetic material arranged outside the screen reaches the magnetic field generated by the conductor of the cable and causes a further increase in the inductance of the conductor, that is to say a further increase in its electrical impedance.
  • This effect of the layer of ferromagnetic material is further increased by re-magnetization losses arising in the same when the superconducting cable is an AC cable.
  • the ferromagnetic material also shields the magnetic field of the conductor of the cable to the outside. Electromagnetic interference for aggregates located outside the cryostat can therefore hardly occur. In addition, forces acting on nearby other cable phases are reduced.
  • the layer of ferromagnetic material may be disposed on the outer circumference of the cryostat.
  • the outer tube of the cryostat itself may advantageously consist of the ferromagnetic material.
  • a material having a high relative permeability ⁇ r is preferably used. It can be used both a material with high Hyteresemaschineen and a material with low hysteresis losses, depending on the desired cable behavior in the short circuit current case.
  • the layer of ferromagnetic material is like all metallic materials also electrically conductive. It can therefore be heated by magnetic hysteresis and by eddy currents under the action of an alternating magnetic field, if any, from the conductor of the cable.
  • this heating occurs in the preferred embodiment of the arrangement outside of the cryostat, so that the cable itself and the cooling medium are not heated thereby. Due to the thus low heating the re-cooling times are reduced, so that the cable is faster again operational. The lower heating also means less mechanical stress on the various components of the assembly. Finally, the coolant remains unaffected by the heating of the ferromagnetic layer. In addition, since only a small cooling capacity is required because of the reduced short-circuit current, the design of the cooling system can be simplified in this preferred embodiment of the arrangement.
  • the layer of ferromagnetic material is heated only insignificantly by an alternating field which may be generated by the conductor of the cable.
  • a material advantageously has a high relative permeability ⁇ r .
  • the layer of ferromagnetic material can be arranged in particular in such a material and within the cryostat. It can then, for example, directly surround the screen of the cable. It could also be the inner tube of the cryostat made of the ferromagnetic material in this embodiment of the cable.
  • the arrangement is according to Fig. 1 from a superconducting cable SK and a cryostat KR surrounding the same.
  • the cryostat KR also includes a free space FR through which a coolant is passed during operation of the arrangement, for example nitrogen.
  • the superconducting cable SK consists of a superconducting conductor 1, a dielectric 2 surrounding it, acting as insulation, and a superconducting screen 3 arranged above the dielectric 2.
  • the cryostat KR is constructed of two concentrically arranged metallic tubes 4 and 5, which are preferably made of steel and can be corrugated transversely to their longitudinal direction to improve the flexibility of the cryostat. Between the inner tube 4 and the outer tube 5 of the cryostat KR a vacuum insulation 6 is mounted in a known technique.
  • the conductor 1 and the screen 3 have superconductive materials. They are in the superconducting state with appropriate cooling during operation of the cable SK. However, the materials of conductor 1 and screen 3 are different, and although in such a way that in the normal conducting state, the material of the screen has a by a factor of at least 50 greater electrical resistance than the material of the conductor. 1
  • the screen 3 consists for the most part advantageously of a rare earth doped, oxide superconductive material.
  • a rare earth doped, oxide superconductive material is known as ReBCO (rare earth barium copper oxide).
  • a material preferably used for the screen 3 is YBCO.
  • the conductor 1 is advantageously made of BSSCO and optionally of an electrical and mechanical stabilization of copper. Because of the high silver content in the BSSCO, the conductor 1 in the normal conducting state has a much lower electrical resistance than the shield 3. This effect can be achieved even if a combination of ReBCO, preferably YBCO, and copper is used for the conductor 1.
  • the shield 3 of the cable SK loses its shielding function as far as possible.
  • the magnetic field generated by the conductor 1 of the cable SK can thereby propagate almost unhindered and directly causes a substantial increase in the inductance of the conductor 1, ie an increase in its electrical impedance.
  • the current flowing through the conductor 1 short-circuit current is characterized significantly and quickly limited.
  • the heat generated by the short-circuit current of the cable SK and its surroundings is thus kept relatively low, so that the energy required for the re-cooling of the device after the short circuit is relatively low.
  • the cable SK can according to the FIGS. 2 and 3 additionally comprise a layer of ferromagnetic material disposed outside the screen 3:
  • Fig. 2 is mounted over the outer tube 5 of the cryostat KR a tubular closed layer 7 of ferromagnetic material. She is on the present throughout the length of the assembly and surrounding the tube 5 at its periphery all around.
  • the layer 7 is thus a tubular closed shell. It reaches in the case of a short circuit in the magnetic field generated by the conductor 1 of the cable SK and thereby causes an additional increase in the inductance of the conductor 1, that is, a further increase in its electrical impedance.
  • the effects explained above are thus enhanced by the layer 7 of ferromagnetic material.
  • the superconducting cable SK is an AC cable, the effect limiting the short-circuit current can be further increased by re-magnetization losses possibly occurring in the layer 7 of ferromagnetic material.
  • the layer 7 could also be made from a longitudinal inlet band of such a material which completely surrounds the tube 5 with a longitudinal overlapping point.
  • the wall thickness of the layer of ferromagnetic material is advantageously greater than 0.1 mm.
  • the relative permeability ⁇ r of the ferromagnetic material is greater than 10.
  • Ferromagnetic materials are generally characterized by a high relative permeability ⁇ r . Independently, ferromagnetic materials have hysteresis losses due to the enclosed area in the BH diagram. Both sizes depend on the material used. There is no correlation between ⁇ r and the hysteresis losses.
  • the layer of ferromagnetic material is arranged in all embodiments as a completely closed layer outside of the superconductive screen 3 so that it lies in the short-circuit case in the magnetic field of the conductor 1. It can accordingly according Fig. 3 can also be arranged within the cryostat KR and rest as a layer 8, for example on the outside of the screen 3. As already mentioned, a material with very low hysteresis losses is advantageously used for the layer 8, so that the same is heated only insignificantly in the event of a short circuit. The layer 8 can then be connected to the same potential as the screen 3. Instead of the separate layer 8 can - analogous to Fig. 1 - Be the inner tube 4 of the cryostat KR made of ferromagnetic material. Also in this embodiment of the arrangement with lying within the cryostat KR ferromagnetic material results in the limitation of the current flowing in the conductor 1 short-circuit current, as for the arrangement according to Fig. 1 is described.

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)
  • Containers, Films, And Cooling For Superconductive Devices (AREA)
EP08291180A 2008-12-15 2008-12-15 Anordnung mit einem supraleitfähigen Kabel Not-in-force EP2202762B1 (de)

Priority Applications (8)

Application Number Priority Date Filing Date Title
AT08291180T ATE498184T1 (de) 2008-12-15 2008-12-15 Anordnung mit einem supraleitfähigen kabel
DK08291180.1T DK2202762T3 (da) 2008-12-15 2008-12-15 Anordning med et supraledende kabel
DE502008002580T DE502008002580D1 (de) 2008-12-15 2008-12-15 Anordnung mit einem supraleitfähigen Kabel
EP08291180A EP2202762B1 (de) 2008-12-15 2008-12-15 Anordnung mit einem supraleitfähigen Kabel
US12/623,849 US9496072B2 (en) 2008-12-15 2009-11-23 Arrangement having a superconducting cable
JP2009269977A JP5632152B2 (ja) 2008-12-15 2009-11-27 超伝導ケーブルを備える装置
KR1020090124282A KR101657600B1 (ko) 2008-12-15 2009-12-14 초전도 케이블을 갖는 구조체
CN2009102614492A CN101752036B (zh) 2008-12-15 2009-12-15 具有超导线缆的装置

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
EP08291180A EP2202762B1 (de) 2008-12-15 2008-12-15 Anordnung mit einem supraleitfähigen Kabel

Publications (2)

Publication Number Publication Date
EP2202762A1 EP2202762A1 (de) 2010-06-30
EP2202762B1 true EP2202762B1 (de) 2011-02-09

Family

ID=40386531

Family Applications (1)

Application Number Title Priority Date Filing Date
EP08291180A Not-in-force EP2202762B1 (de) 2008-12-15 2008-12-15 Anordnung mit einem supraleitfähigen Kabel

Country Status (8)

Country Link
US (1) US9496072B2 (ja)
EP (1) EP2202762B1 (ja)
JP (1) JP5632152B2 (ja)
KR (1) KR101657600B1 (ja)
CN (1) CN101752036B (ja)
AT (1) ATE498184T1 (ja)
DE (1) DE502008002580D1 (ja)
DK (1) DK2202762T3 (ja)

Families Citing this family (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2426676A1 (de) * 2010-09-02 2012-03-07 Nexans Anordnung mit mindestens einem supraleitfähigen Kabel
JP5598718B2 (ja) * 2010-12-28 2014-10-01 住友電気工業株式会社 多層絶縁継手及び二重管の接続構造
EP2690737B1 (de) * 2012-07-25 2017-08-30 Nexans Anordnung mit drei supraleitfähigen Phasenleitern
JP6200402B2 (ja) * 2014-03-06 2017-09-20 住友電気工業株式会社 超電導ケーブル線路、及び断熱管路
US10141744B2 (en) * 2016-05-17 2018-11-27 General Electric Company Cable arrangement of an energy storage system
RU2745404C2 (ru) * 2016-05-26 2021-03-24 Тюбу Юниверсити Эдьюкейшнл Фаундейшн Способ установки сверхпроводящего кабеля и кабельный каркас
DK3402000T3 (da) * 2017-05-12 2020-05-11 Nexans Anordning til forbindelse af superledende kabler
CN108039248B (zh) * 2017-12-08 2020-08-14 北京原力辰超导技术有限公司 一种带复合电磁屏蔽层的高温超导缆线
WO2022108820A1 (en) 2020-11-18 2022-05-27 VEIR, Inc. Conductor systems for suspended or underground transmission lines
AU2021381889A1 (en) 2020-11-18 2023-06-08 VEIR, Inc. Systems and methods for cooling of superconducting power transmission lines
AU2021381750A1 (en) 2020-11-18 2023-06-08 VEIR, Inc. Suspended superconducting transmission lines

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JPS58147906A (ja) * 1982-02-25 1983-09-02 富士通株式会社 電力ケ−ブル
JPS63241807A (ja) * 1987-03-27 1988-10-07 Sumitomo Electric Ind Ltd 高忠実度信号伝送用電線
JP3117519B2 (ja) * 1991-12-07 2000-12-18 株式会社フジクラ 酸化物超電導線材
JPH06275146A (ja) * 1993-03-18 1994-09-30 Hitachi Ltd 複合超電導線材
JP3342739B2 (ja) * 1993-05-10 2002-11-11 株式会社フジクラ 酸化物超電導導体とその製造方法およびそれを備えた酸化物超電導電力ケーブル
JP4667644B2 (ja) 2001-05-29 2011-04-13 古河電気工業株式会社 超電導ケーブル
AU2002222365A1 (en) 2001-12-17 2003-06-30 Pirelli & C S.P.A. Electric power transport system comprising a cold dielectric sup erconducting cable
JP4298450B2 (ja) * 2003-09-24 2009-07-22 住友電気工業株式会社 超電導ケーブルの端末構造
JP4880229B2 (ja) * 2005-01-31 2012-02-22 株式会社ワイ・ワイ・エル 超伝導送電ケーブル及び送電システム
JP5115778B2 (ja) * 2006-01-16 2013-01-09 住友電気工業株式会社 超電導ケーブル
KR100706494B1 (ko) * 2006-01-20 2007-04-10 엘에스전선 주식회사 초전도 케이블
JP2007265919A (ja) * 2006-03-29 2007-10-11 Sumitomo Electric Ind Ltd 導体引出構造
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JP4967750B2 (ja) * 2007-03-28 2012-07-04 住友電気工業株式会社 超電導ケーブルの接続構造および超電導ケーブルの接続方法
JP5018502B2 (ja) * 2008-01-18 2012-09-05 住友電気工業株式会社 超電導ケーブル
CN101246767B (zh) * 2008-03-26 2011-07-27 华北电力大学 一种高温超导电缆或母线本体的设计方法

Also Published As

Publication number Publication date
EP2202762A1 (de) 2010-06-30
DE502008002580D1 (de) 2011-03-24
CN101752036A (zh) 2010-06-23
US20100152049A1 (en) 2010-06-17
JP2010161064A (ja) 2010-07-22
ATE498184T1 (de) 2011-02-15
JP5632152B2 (ja) 2014-11-26
KR20100069602A (ko) 2010-06-24
CN101752036B (zh) 2013-11-27
DK2202762T3 (da) 2011-05-23
KR101657600B1 (ko) 2016-09-19
US9496072B2 (en) 2016-11-15

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